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The reason that it's so hard to understand what physicists mean when they talk about "gauge freedom" is that there are at least four inequivalent definitions that I've seen used:
Definition 1: A mathematical theory has a gauge freedom if some of the mathematical degrees of freedom are "redundant" in the sense that two different mathematical expressions ...
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Gauge symmetries, as the note says, are redundancies in our description of nature. For example, a photon has two physical degrees of freedom (the two polarizations). However, we choose to describe a photon using a 1-form field $A_\mu$ which has 4 degrees of freedom. The two extra degrees of freedom here are related to gauge symmetries. From here on, there ...
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You're making some category errors in the question. Energy can't be converted into mass, mass is a form that energy can take. In other words, when energy is "converted" into mass it never stops being energy. It's kind of like if I have a mass on a spring hanging vertically in a gravitational field, and I make it start bouncing. The energy moves back and ...
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A theory is typically described by a Lagrangian, and varying this gives us the equations of motion of the system. The symmetries you describe are symmetries of the Lagrangian i.e. they are transformations that leave the Lagrangian unchanged.
It would be nice to think that the Lagrangians that describe our leading theories of physics were derived in some ...
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The first answer to such a question must always be: A gauge symmetry has no "physical" meaning, it is an artifact of our choice for the coordinates/fields with which we describe the system (cf. Gauge symmetry is not a symmetry?, What is the importance of vector potential not being unique?, "Quantization of gauge systems" by Henneaux and Teitelboim). Any ...
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Since you mentioned coming from a mathematics background, you might find it nice to take an answer in terms of equivalence classes.
A gauge theory is physical theory where the observable quantities, as in, things you could measure with an experiment given perfect measuring equipment, are equivalence classes in a vector space.
Electromagnitism is the most ...
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I only understood this after taking a class in general relativity (GR), differential geometry and quantum field theory (QFT). The essence is just a change of coordinates systems that needs to be reflected in the derivative. I'll explain what I mean.
You have a theory that is invariant under some symmetry group. So in quantum electrodynamics you have a ...
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The identification goes as follows:
$$ \text{Kin. Mom.}~=~ \text{Can. Mom.} ~-~\text{Charge} \times \text{Gauge Pot.} $$
$$ \updownarrow $$
$$ m\hat{v}_{\mu} ~=~ \hat{p}_{\mu} - qA_{\mu}(\hat{x})$$
$$ \updownarrow $$
$$ \frac{\hbar}{i} D_{\mu} ~=~ \frac{\hbar}{i}\partial_{\mu} - qA_{\mu}(x) $$
$$ \updownarrow $$
$$ D_{\mu} ~=~ \partial_{\mu} -\frac{...
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The fact that the theory is not gauge invariant implies that all degrees of freedom of $A_\mu$ must have physical meaning: This is not the theory of photons where only transverse degrees of freedom make sense.
This way you must tackle some non-trivial issue like the negative norm associated with temporal modes. This could be avoided by adding a mass to $A_\...
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Here we will assume that we ultimately want to consider the full quantum theory, usually written in terms of a gauge-fixed path integral
$$Z~=~\int \!{\cal D}\phi~ \exp\left(\frac{i}{\hbar}S_{\rm gf}[\phi]\right) \tag{1}$$
rather than just the classical action and the corresponding classical equations of motion (with or without gauge-fixing terms). If the ...
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They require a special discussion because they are different. The (defining) fact that they can't be deformed to the identity means that it is not enough to verify the invariance under infinitesimal gauge transformations: the problem is that the large gauge transformations cannot be obtained by combining many infinitesimal gauge transformations!
The modular ...
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Comments to the question (v1):
Last thing first. On-shell means (in this context) that equations of motion (eom) are satisfied. Equations of motion means Euler-Lagrange equations. Off-shell means strictly speaking not on-shell, but in practice it is always used in the sense not necessarily on-shell. [Let us stress that every infinitesimal transformation is ...
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OP has a point. The field $A^\mu$ is a connection, and therefore it lives in the algebra of the gauge group, not in the group itself. In this case, $\mathfrak u(1)=\mathbb R$. At first sight, this is all we may conclude from $A\to A+\mathrm d\Lambda$. The group $\mathrm U(1)$ is, apparently, not here yet.
The correct statement is that the theory described ...
answered Jan 29 '18 at 15:56
AccidentalFourierTransform
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The change of the overall phase of the wave function
$$ |\psi \rangle \to e^{i\phi} |\psi\rangle $$
has no physical implications. However, the change of the relative phase of two terms in the wave function always has physical consequences. In particular, in the Bohm-Aharonov effect, the particle may avoid the solenoid on the left side or the right side – ...
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$\chi$ is a real-valued function. This is part of the definition of the gauge transformation, since $U(1)$ is a one (real) dimensional group. In general, when talking about gauge transformations in particle physics, group parameters are restricted to be real by convention.
In principle, I suppose you could perform a transformation on the wavefunction that ...
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The guiding principle is: "Anomalous symmetries cannot be gauged". The phenomenon of anomalies is not confined to quantum field theories. Anomalies exist also in classical field theories (I tried to emphasize this point in my answer on this question).
(As already mentioned in the question), in the classical level, a symmetry is anomalous when the Lie ...
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I) Vanishing field-strength $F=0$ does not imply that the gauge potential $A$ is pure gauge. It only holds locally. There could be global obstructions. In fact, topological obstructions could happen even if the gauge group $G$ is Abelian.
II) Let us sketched the proof of the local statement in a sufficiently small neighborhood $\Omega\subseteq M$ of a point ...
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Comment to the question (v1): It seems OP is conflating, on one hand, a gauge transformation
$$ \tilde{A}_{\mu} ~=~ A_{\mu} +d_{\mu}\Lambda $$
with, on the other hand, a gauge-fixing condition, i.e. choosing a gauge, such e.g., Lorenz gauge, Coulomb gauge, axial gauge, temporal gauge, etc.
A gauge transformation can e.g. go between two gauge-fixing ...
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Gauge invariance is simply a redundancy in the description of a physical system. I.e. we can choose from an infinite number of vector potentials in E&M.
For example, an infinite number of vector potentials can describe electromagnetism by the transformation below
$$A(x) \to A_\mu(x) + \partial_\mu \alpha(x)$$
Choosing a specific gauge (gauge fixing) ...
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These calculations very often depend only on the difference between two values, not the concrete values themselves. You are therefore free to choose a zero to your liking. Is this an example of gauge invariance in the same sense as the graduate examples above?
Yes indeed it is, in the most general definition of gauge invariance, it's what physicists call a ...
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Bundles and compactified spacetime
A gauge theory cannot be looked at purely locally, it has inherently global features on cannot see locally. The proper mathematical formalization of a Yang-Mills gauge theory is that the gauge field $A$ is a connection on a principal bundle $P\to M$ over spacetime $M$. However, in practice, it turns out that physicists don'...
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We do not start from the assumption that the Lagrangian "should" be invariant under gauge transformations. This assumption is often made because global symmetries are seen as more natural than local symmetries and so writers try to motivate gauge theory by "making the global symmetry local", but this is actually nonsense. Why would we want a local symmetry ...
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You seem to be mixing up a few different things. The Standard Model does not say the up and down quark must have the same mass.
The up and down quark form a doublet of the flavor symmetry $SU(2)_F$. This is an approximate symmetry that is broken explicitly by the up and down quark mass difference.
The left-handed up and down quarks form a doublet $Q_L$ of ...
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I) In general, it is true that if we plug a local Lagrangian
$$\tag{1} L\quad \longrightarrow \quad \tilde{L}~=~L+\frac{df}{dt}$$
modified with a total derivative term into the Euler-Lagrange expression
$$\tag{2} \sum_{n} \left(-\frac{d}{dt}\right)^n \frac{\partial \tilde{L}}{\partial q^{(n)}}~=~\sum_{n} \left(-\frac{d}{dt}\right)^n \frac{\partial L}{\...
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Multiplying by $e^{i\theta}$ is a rotation of $\theta$ in the complex plane. Physically it changes the phase of a plane wave by an angle $\theta$. This is a global symmetry because we arbitrarily choose a reference point for measuring the phase of plane waves. If we change the phase of all plane waves by an equal amount then this is equivalent to just moving ...
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The statement
because the gauge transformation is not supposed to change anything, it means that every expectation can be calculated equivalently using $ \psi' $ or $ \psi $
isn't particularly correct. All physically measurable expectation values can be calculated correctly in any arbitrary gauge, but the operator representation of some operators can ...
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A free "$\mathrm{U}(1)$" gauge theory can never tell whether the gauge group is $\mathrm{U}(1)$ or $\mathbb{R}$ because the only field in the theory, the gauge potential $A$, transforms as
$$ A\mapsto A + \partial_\mu \chi,$$
where $\chi$ is just a real-valued function, and the real numbers are the Lie algebra of both $\mathrm{U}(1)$ and $\mathbb{R}$. This ...
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GR has some formal resemblance to Yang-Mills gauge theory. But it isn't quite the same thing.
We formulate YM in terms of gauge fields, AKA, connections on G-bundles on our manifold. We also make use of a connection when we formulate GR, the Levi-Civita connection on the tangent bundle of our spacetime, which is determined by the metric and some ...
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Your proposed definitions are not quite correct. I'll sketch correct definitions, but I won't actually give them because I don't know how you choose to define classical field theory.
A group of local symmetries is a group of symmetry transformations where you get to change the system differently at different places in space/time.
A symmetry is global (in ...
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